Curvature insensitive gradient index multi-more light conducting fiber

ABSTRACT

The invention relates to a bend insensitive gradient index multimode light conducting fiber comprising a leakage mode dependent optical core diameter that is uniform over its length and a numerical aperture that is uniform over its length, a core ( 1 ), an inner cladding ( 2 ), a refraction index trench ( 3 ) and an outer cladding ( 4 ), wherein the core ( 1 ) includes a core radius R 1,  an alpha-refraction index profile and a core refraction index difference dn 1  with respect to the outer cladding ( 4 ), wherein the refraction index trench ( 3 ) includes a refraction index trench radius R 3  and a trench refraction index difference dn 3  with respect to the outer cladding ( 4 ), wherein the outer cladding ( 4 ) includes an outer cladding radius R 4  and a refraction index between 1.40 and 1.55, wherein for a light wavelength of 850 nm and an overfilled launch (OFL), the optical core diameter for a fiber length in a range between 2 m and 300 m decreases by less than 5% and the numerical aperture decreases by less than 2.5% and the curvature related attenuation increase for two turns and a curvature radius of 7.5 mm is less than 0.2 db.

The invention relates to a bend insensitive gradient index multi-mode light conducting fiber according to the preamble of patent claim 1.

A standard gradient index multimode light conducting fiber subsequently designated as GIMM-fiber includes a fiber core with a so-called alpha-refraction index profile, wherein the refraction index difference of the core relative to a surrounding cladding essentially s a power function of the radius. The core is made from doped silica and the cladding is preferably made from non-doped fused silica. Fibers of this type have already been used for many years.

It is known that the so-called macro-bend losses of fibers of this type can be reduced by inserting a so-called refraction index trench between the center core and the surrounding cladding. The refraction index trench is a portion in which the refraction index is lowered relative to the core and also relative to the cladding. Fibers of this type are also designated as bend insensitive multimode fibers with the abbreviation BIMMF. The macro-bend properties of such BIMMF with respect to an attenuation increase, the measured wavelength, the number of turns and the bend radius is described in standardized international specifications.

It is a consequence of the trench concept to reduce the macro-bend losses that in a BIMM light conducting fiber so-called leakage modes are also generated as a function of excitation conditions besides the typically occurring propagation capable modes, One of these frequently occurring excitation types is designated as overfilled launch excitation (OFL excitation). For an excitation of this type, the directly light conducting core of the light conductor fiber is overfilled through excitation with a light source. In OFL excitations, leakage modes are generated which can propagate over several hundred meters.

In standard GIMM light conducting fibers without the recited trench concept leakage modes can only be observed over a length of a few millimeters from the coupling location and they do not have any practical significance. In BIMMF with trench structure, the leakage modes, however, are run through the refraction index trench over a longer distance. This means that the increase in insensitivity relative to macro-bends which is obtained through the trench concept of the BIMMF over the standard GIMM light conducting fibers causes a disadvantage through leakage mode conduction, in particular for an OFL excitation.

This leakage mode conduction has negative impacts on the optical properties of the light conducting fibers which depend from the fiber length. GIMM light conducting fibers are defined with respect to their light conducting properties through the parameter of the optical core diameter and the numerical aperture. Thus, an excitation over the entire diameter of the geometric fiber core is presumed. The geometric fiber core is defined by the configuration of the light conducting fiber. The optical core diameter contrary thereto describes the portion of the fiber core that is effectively usable for light conduction.

Thus, the optical core diameter decreases with increasing length of the light conducting fiber. This is caused by the leakage modes described supra which exit from the fiber core and which limit the core diameter of the light conducting fiber that is actually suitable for light conduction with increasing fiber length. This leakage mode attenuation is independent from the so-called fiber base attenuation which occurs due to the fiber material. The leakage mode attenuation practically exclusively depends from the refraction index distribution in the fiber core and generally also in the fiber cross-section.

The length dependency of the optical core diameter and of the numerical aperture caused by the leakage modes is also independent from the actually provided macro-bend of the light conducting fiber and thus also dependent from its installation type. Fiber bends are typically designated as macro-bends in which the fiber axially deviates from a straight line with a bend radius in the dm, cm, or mm range. Macro-bend losses do not result from leakage mode conduction, but are partially caused by modes of higher order which are not run in the core anymore for increasing bending so that their power portion is emitted and therefore lost. Furthermore, macro-bends attenuate each mode that is run in the fiber because the electromagnetic field reaches into the fiber cladding further in the outside. This attenuation increase is the larger, the smaller the bending radius of the fiber and the greater the wavelength of the conducted light. The longitudinal dependency of the optical core diameter caused by leakage modes, however, also occurs when the fiber is oriented completely straight.

Thus, a light conducting fiber can be provided which shows little sensitivity relative to macro-bends. However, this introduces high leakage mode conduction into the light conducting fiber which regardless of the installation mode of the light conducting fiber, can only be influenced very little.

Due to the leakage mode attenuation, the optical core diameter with increasing fiber length reaches a substantially constant value, however, the coupling properties of the light conducting fiber are degraded through this damping effect and additionally depend from the length of the light conducting fiber.

For bend insensitive light conducting fibers, therefore, the smallest possible change of the optical core diameter and the numerical aperture as a function of the fiber length is desirable. In order to characterize the dependency of the optical core diameter from the fiber length, a measuring procedure is used that is defined according to the international GIMMF standard. Thus, the optical core diameter is determined at a 2 m long fiber piece through a standard measurement and compared with the optical core diameter at a second fiber length, for example for 300 or 1,000 m, Typically, fiber lengths are selected in which the length dependency of the optical core diameter becomes clearly apparent.

Another problem when using the BIMM fibers is that the parameters that are important for a specification of the fiber and for determining fiber-, splicing- and coupling-losses like e.g. the optical core diameter or its NA cannot be determined in a simple manner. The fiber parameters determined through OFL, excitation using measurement methods configured for standard GIMM fibers have proven too large for applications to BIMM fibers. This leads to misinterpretations with respect to the splicing and coupling losses that shall be estimated and also for compatibility considerations of the measurement values compared to standard GIMM fibers.

Thus, it is an object of the invention to provide a GIMM light conducting fiber which is insensitive against bending which has a configuration under the conditions of the occurring leakage modes which provides the smallest length dependency of the optical core diameter that is possible. It shall be facilitated on the one hand side to provide a light conducting fiber which is sufficiently insensitive against macro-bends in which, however, on the other hand side the leakage mode propagation is substantially minimized. This relates in particular to providing the best possible parameters for the optical core diameter and the numerical aperture of the light conducting fiber for OFL excitations while simultaneously complying with minimum requirements for macro-bending.

This object is achieved with a bend insensitive GIMM light conducting fiber with the features of claim 1.

The bend insensitive GIMM light conducting fiber with an optical core diameter and a numerical aperture includes a core, an inner cladding, a refraction index trench and an outer cladding. It is characterized in that the core includes a core radius, an alpha refraction index profile and a core refraction index difference with respect to the outer cladding. The refraction index trench has a trench radius and a trench refraction index difference with respect to the outer cladding and the outer cladding has an outer cladding radius and a refraction index between 1.40 and 1.55, wherein the parameters are set so that for a light wavelength of 850 nm and a overfilled launch (OFL) the optical core diameter for a fiber length in a range from 2 m to 300 m is reduced by less than 5% and the numerical aperture is reduced by less than 2.5% and the bend related attenuation increase for two turns and a bend radius of 7.5 mm is less than 0.2 dB.

The fiber configuration according to the invention of the bend insensitive GIMM light conducting fiber is thus based on a core with an alpha refraction index profile and combines this core with a refraction index trench and a cladding enveloping the core. Thus, the core has a positive refraction index difference from the surrounding cladding, wherein the refraction index trench has a lower refraction index compared to the cladding. The basic idea of the fiber configuration according to the invention is to adjust the dimensions of the core, the refraction index trench and of the cladding so that the lowest possible length dependency of the optical core diameter and of the numerical aperture is achieved. Thus, the curvature related attenuation increase is lowered under the recited value.

In an advantageous embodiment of the fiber configuration, the core is enveloped by an inner cladding, wherein the inner core includes an inner cladding radius and an inner cladding refraction index difference relative to the outer cladding.

In an advantageous embodiment, the inner cladding refraction index difference has a value of 2*10̂−3 to 3*10̂−3 relative to the outer cladding.

Furthermore, an inner cladding with a width B can be provided in the refraction index profile between the core and refractive index trench. The inner cladding width in one embodiment is 1 to 5 μm.

In an advantageous embodiment, the core has a geometric core diameter between 48 and 50 μm for a numerical core aperture of 0.18 to 0.22 and a core refraction index difference between 12*10̂−3 and 17*10̂−3 relative to the outer cladding. Thus, the refraction index difference of the inner cladding relative to the outer cladding is 0, the width of the refraction index trench is between 2 and 5 μm and the depth of the refraction index trench is (−6 to −11)*10̂−3.

In another embodiment, the core includes a core refraction index step, wherein the ore refraction index step has a value between (−1.0 and 1.0)*10̂−3.

The total fiber diameter in one embodiment is between 120 and 130 μm.

Furthermore, an outer coating can be provided that envelops the light conducting fiber, wherein the diameter of the coating is 230 to 510 μm.

The bend insensitive GIMM light conducting fibers according to the invention shall be subsequently described in more detail with reference to an exemplary embodiment. FIGS. 1 through 3 are being referred to. The same reference numerals are being used for identical or equivalent components in the drawing figures, wherein:

FIG. 1 illustrates a first exemplary refraction index profile with a gradient index core and a refraction index trench;

FIG. 2 illustrates a second exemplary refraction index profile with a gradient index core and with a core refraction index step, an inner cladding directly joining the core and a refraction index trench connected thereto; and

FIG. 3 illustrates a third refraction index profile with a gradient index core and an inner cladding with an inner cladding refraction index difference relative to the outer cladding.

FIG. 1 illustrates a first exemplary refraction index profile of the bend insensitive GIMM light conducting fiber. The depiction illustrates the refraction index difference relative to a reference value as a function of the radius of the light conducting fiber. The light conducting fiber has a core 1 with a so-called alpha-refraction index profile. The general diagram of the refraction index difference is defined for example by the formula:

${\Delta \; {n(R)}} = {{dn}\; {1 \cdot \left( {1 - \left\lbrack \frac{R}{R\; 1} \right\rbrack^{\alpha}} \right)}}$

Therein dn1 is the refraction index difference in the center of the fiber for R=0, R1 is the core radius and a is the so-called profile exponent. The diagram of the core profile defined by this formula describes an approximation of the actually produced profile distribution. For further illustrations, the deviation of the actual refraction index diagram from the ideal refraction index diagram is of subordinate importance, since the deviations are typically very small in modern GIMM light conducting fibers.

The core 1 is enveloped by an inner cladding 2 and a trench 3. An outer cladding 4 adjoins the trench in outward direction. The inner cladding has a radius R2, the trench has a radius R3 and a trench width b. The refraction index of the trench is reduced relative to the refraction index of the outer cladding and is visible in the profile as a trench depth dn3.

It is apparent in the instant first embodiment that the inner cladding 2 is at the same refraction index level as the outer cladding 4. An exemplary fiber design with the instant refraction index profile has for example the following values:

R1 ˜24 μm, R2 ˜27 μm; core-NA ˜0.20; dn1 ˜13.8*10̂−3; b ˜3 μm; dn3 ˜−9*10̂−3; the radius of the entire fiber ˜62.5 μm with a radius of a surrounding coating of approximately 122 μm.

FIG. 2 illustrates another embodiment. At the beginning of the core at R1, there is a core refraction index step 1 a with a core refraction index step in the amount of dn4. The care refraction index step dn4 refers to the outer cladding refraction index and can have positive values (0 to 1*10̂−3) and also negative values (0 to −1*10̂−3). The core radius R1 and the core refraction index dn1 essentially correspond to the embodiment of FIG. 1. Also for this fiber design, the core 1 is enveloped by an inner cladding 2 and a trench 3. The inner cladding 2 has a radius R2, the trench radius is R2.

FIG. 3 illustrates an embodiment in which the inner cladding has a lower refraction index level than the outer cladding. Thus, an inner cladding refraction index difference dn2 is provided with respect to the outer cladding. Exemplary values for dn2 are in the range of 2*10̂−3 to approx. −3*10̂−3. In the embodiment of FIG. 3, all other parameters can be configured essentially like in the embodiment of FIG. 1.

The light conducting fiber according to the invention was described based on exemplary embodiments. Further embodiments can be derived from the dependent claims. Additional variations are apparent to a person skilled in the art. 

1. A bend insensitive gradient index multimode light conducting fiber comprising a leakage mode dependent optical core diameter that is uniform over its length and a numerical numerical aperture that is uniform over its length, a core, an inner cladding, a refraction index trench and an outer cladding, wherein the core includes a core radius R1, an alpha-refraction index profile and a core refraction index difference dn1 with respect to the outer cladding, wherein the refraction index trench includes a refraction index trench radius R3 and a trench refraction index difference dn3 with respect to the outer cladding, wherein the outer cladding includes an outer cladding radius R4 and a refraction index between 1.40 and 1.55, wherein for a light wavelength of 850 nm and an overfilled launch (OFL), the optical core diameter for a fiber length in a range between 2 m and 300 m decreases by less than 5% and the numerical aperture decreases by less than 2.5% and the curvature related attenuation increase for two turns and a curvature radius of 7.5 mm is less than 0.2 db.
 2. The light conducting fiber according to claim 1, wherein the core is enveloped by an inner cladding, wherein the inner cladding includes an inner cladding radius R2 and an inner cladding refraction index difference dn2 with respect to the outer cladding.
 3. The light conducting fiber according to claim 2, wherein the inner cladding refraction index difference dn2 has a value of 2*10̂−3 to −3*10̂−3 with respect to the outer jacket cladding.
 4. The light conducting fiber according to claim 2, wherein the difference of the inner cladding radius R2 and the core radius R1 is 1 to 5 μm.
 5. The light conducting fiber according to claim 1, wherein the core has a geometric core diameter between 48 and 50 μm for a numerical numerical core aperture between 0.18 and 0.22 and a core refraction index difference between 12*10̂−3 and 17*10̂−3, an inner cladding refraction index difference of 0, a width of the refraction index trench of 2 to 5 μm and a depth of the refraction index trench of (−6 to −11)*10̂−3.
 6. The light conducting fiber according to claim 1 wherein the core has a core refraction index step in the amount of dn4, wherein the core refraction index step has a value between (−1.0 and 1.0)*10̂−3.
 7. The light conducting fiber according to claim 1, wherein a total diameter of the fiber is between 120 and 130 μm
 8. The light conducting fiber according to claim 1, wherein an outer coating is provided that envelops the light conducting fiber, wherein the diameter 15 of the coating is 230 to 510 μm. 